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    EEE 313: Electrical Properties ofMaterial

    Textbook: Principles of Electronic

    Materials and Devices (3rdEdition)

    - S.O. Kasap

    1EEE 313

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    Lecture-11

    Elementary Quantum Physics(contd.)

    Course Instructor:Lecturer, EEE, Faculty of E&T

    Eastern University

    2EEE 313

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    Topics:

    Electron as a wave: De Broglie relationship

    Time independent Schrodinger equation

    Infinite potential well: A confined electron

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    The electron as a wave

    DE BROGLIE relationship

    De Broglie relationship relates the wave-like

    properties (e.g. wavelength ) of matter to its particle-

    like properties (e.g. momentum p) via = h/p

    Problem-1: A 50 gram golf ball travelling at a

    velocity of 20 ms-1 , calculate the wave length.

    4EEE 313

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    Under certain conditions , electron exhibits wave like

    properties. The general equation that describes the wave like

    behavior and with the appropriate potential energy and

    boundary conditions will predict the result of the

    experiments, is called the Schrdinger equation.

    The wave function can be written as (x,t).

    In three dimension (x,y,z,t) represent the wave property of

    electron.

    To obtain the wavefunction for electron we need to know how

    electron interact with its environments.

    5

    Time-Independent Schrodinger Equation

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    6

    The time independent Schrdinger equation describes the wave

    behavior of a particle under steady state conditions, i.e.when the

    PEis time independent.The potential energy function is V=V(x,t) ,because the net force the

    electron experiences is F=-dV/dx

    Electrostatic potential energy given by V (r)=

    If potential energy of electron is time independent, the total

    wavefunction of the electron can be written as

    2

    04

    e

    r

    , exp jEt

    x t x

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    Where is the wavefunction of the electron that

    describes only the spatial behavior and E is the total

    energy of the electron. The fundamental equationthat describes the electrons behavior by determining

    is called time independent Schrdinger equation.

    2

    2 2

    2

    0

    d x m

    E V x xd x

    2

    , , ,x y z t is the probability of finding the electron

    per unit volume at x,y,z at time t

    2

    , , ,x y z t dxdydz is the probability of finding the electronin a small elemental volume dx dy dz at

    x,y,z at time t

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    What will be the Schrodingers

    equation for three dimensions??

    [equation 3.16b, page-209]

    8EEE 313

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    Boundary conditions to solve Schrodingers equation

    Two important boundary conditions are often

    used to solve the Schrodinger equation

    (a) (x) must be continuous, single valued &smooth.

    (b) d /dx must be continuous.

    9EEE 313

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    Unacceptable forms of (x)

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    Problems

    Example-3.5: Solve the Schrodinger equation for a

    free electron whose energy is E. What is the

    uncertainty in the position of the electron & the

    uncertainty in the momentum of the electron?[Page-

    211] Example-3.6: Electrons are accelerated through a 100

    V potential difference to strike a polycrystalline

    sample. It has a diffraction angle of 30.4. From X-

    ray studies, the separation of planes is 0.234nm. Whatis the wavelength of the electron and how does it

    compare with that from the de Broglie relationship?

    [Page-212]11EEE 313

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    Infinite Potential Well: A confined electron

    Consider the behaviour of the electron when it is confined to a

    certain region, 0

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    13EEE 313

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    = 0, when x 0 and x a, and is determined by

    the Schrodinger equation in 0 < x < a with V = 0.

    Therefore, in the region 0 < x < a

    d2/ dx2+ (2m E ) /2= 0----- (1)

    This is a 2ndorder linear differential equation. As a

    general solution,(x) = A ejkx + B e -jkxwhere k is some constant(to be determined) and substitute this in equation (1)

    to find k. (0) = 0, therefore, B = -A, so that

    (x) = A [ ejkx - e jkx ] = 2Aj sin (kx) So, equation (1) becomes-

    -2Ajk2(sin kx) + (2m/ 2) E (2Aj sin (kx)) = 0

    14EEE 313

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    Energy of the electron :E = (2k2)/2m

    Wave-function in infinite PE well,

    n(x) = 2Aj sin (nx/a) Electron energy in infinite PE well is,

    En = h2n2/ (8ma2)where n = 1,2,3

    are called eigen-energies of the system.

    What is the value of A???

    To find the value of A, we will use normalization

    condition. Applying this condition, we get

    A = (1/2a) The resulting wave-function for the electron is,

    n(x) = j (2/a)1/2sin (nx/a)

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    Energy separation in infinite PE well

    Energy differences between two consecutive

    energy levels is ,

    E = En+1

    - En

    = h2(2n + 1)/ (8ma2)

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    Problems

    Example-3.7: Consider an electron in an infinite

    potential well of size 0.1 nm. What is the groundenergy of the electron? What is the energy required to

    put the electron at the third energy level? How can

    this energy be provided?[Page-216]

    Example-3.8: Consider a macroscopic object 100

    grams (say, an apple) confined to move between two

    rigid walls separated by 1 m. What is the minimum

    speed of the object? What should the quantumnumber n be if the object is moving with a speed 1

    ms-1? What is the separation of the energy levels of

    the object moving with that speed?[Page-217]

    17EEE 313

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    Thank You

    18EEE 313